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Methods of Determining Centroid X‐Ray Wavelengths: CuKα and FeKα

机译:确定质心X射线波长的方法:CuKα和FeKα

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For an exact solution of the Bragg equation it is necessary that there be a one‐to‐one correspondence (equivalence) between the angular measure θ and the wavelength measure λ. Because the aberrations inherent in all x‐ray diffraction profile measurements distort the profile, it is necessary to correct any given measure (peak, centroid, etc.) for all aberrations. The only angular measure of powder diffractometer profiles that can be corrected to a high degree of accuracy is the centroid. To realize the greater accuracy inherent in the centroid method, accurate centroid spectral wavelengths are required. Centroids of CuKα and FeKα two‐crystal spectrometer profiles prepared by Bearden have been calculated and corrected for axial divergence, distortions arising from variation in absorption across the spectral distributions, crystal asymmetry, and other factors. To determine the centroid wavelength it is necessary to truncate the profile; equivalence of λ and θ is maintained by truncating the powder and spectral profiles in the same manner. Four methods for systematically truncating the profiles have been published; the methods are evaluated and the superiority of one of the methods is demonstrated. It is shown that the centroid wavelength is a function of integration (wavelength) range, primarily as a result of inclusion or exclusion of the Kα satellite group within the truncated profile. The two‐crystal spectrometer profiles are compared with models based on a Cauchy distribution. The necessity for additional spectral data before reference centroid wavelengths can be established is discussed.
机译:为了精确地求解布拉格方程,必须在角度量度θ和波长量度λ之间存在一一对应的关系(等效性)。由于所有X射线衍射轮廓测量中固有的像差会使轮廓失真,因此有必要针对所有像差校正任何给定的量度(峰值,质心等)。可以高精度校正的粉末衍射仪轮廓的唯一角度测量是质心。为了实现质心方法固有的更高准确性,需要准确的质心光谱波长。已计算出Bearden制备的CuKα和FeKα双晶体光谱仪轮廓的质心,并针对轴向发散,因光谱分布中的吸收变化而引起的畸变,晶体不对称以及其他因素进行了校正。为了确定质心波长,有必要截断轮廓。通过以相同方式截断粉末和光谱轮廓,可以保持λ和θ的等价性。系统地截断轮廓的四种方法已经发布。对这些方法进行了评估,并证明了其中一种方法的优越性。结果表明,质心波长是积分(波长)范围的函数,主要是由于在截断轮廓内包含或排除了Kα卫星群。将双晶体光谱仪的轮廓与基于柯西分布的模型进行了比较。讨论了在可以确定参考质心波长之前需要附加光谱数据的问题。

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    《Journal of Applied Physics 》 |1964年第4期| 共10页
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  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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